Principles & Applications Operational Amplifiers

Slides:



Advertisements
Similar presentations
Principles & Applications Small-Signal Amplifiers
Advertisements

Chapter 18 Operational Amplifiers. The typical op amp has a differential input and a single-ended output. Class B push-pull emitter follower Diff amp.
Op-amp Circuits and Active Filters
CHAPTER 1: INTRODUCTION TO OPERATIONAL AMPLIFIERS
Ref:080114HKNOperational Amplifier1 Lecture 1 Op-Amp Introduction of Operation Amplifier (Op- Amp) Analysis of ideal Op-Amp applications Comparison of.
Week 6aEECS40, Spring 2005 Week 6a OUTLINE Op-Amp circuits continued: examples Inverting amplifier circuit Summing amplifier circuit Non-inverting amplifier.
Operational Amplifier
Department of Information Engineering357 Operation amplifier The tail, large impedance gives high CMRR Mirror as active load. High gain Follower as buffer.
1 ECE 3336 Introduction to Circuits & Electronics MORE on Operational Amplifiers Spring 2015, TUE&TH 5:30-7:00 pm Dr. Wanda Wosik Set #14.
Chapter 13: Operational Amplifiers
Chapter 10: Operational Amplifiers. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey All rights reserved. Electronic Devices.
Electronics Principles & Applications Sixth Edition Chapter 7 More About Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles A.
© 2012 Pearson Education. Upper Saddle River, NJ, All rights reserved. Electronic Devices, 9th edition Thomas L. Floyd Electronic Devices Ninth.
Introduction to Op Amps
Ch7 Operational Amplifiers and Op Amp Circuits
McGraw-Hill © 2008 The McGraw-Hill Companies Inc. All rights reserved. Electronics Principles & Applications Seventh Edition Chapter 8 Large-Signal Amplifiers.
Principles & Applications Large-Signal Amplifiers
Content Op-amp Application Introduction Inverting Amplifier
Electronics Principles & Applications Sixth Edition Chapter 6 Introduction to Small-Signal Amplifiers (student version) ©2003 Glencoe/McGraw-Hill Charles.
1 The 741 Operational-Amplifier. Reference Bias Current : The 741 op-amp circuit. Reference Bias Current.
Introduction to Op Amp Circuits ELEC 121. April 2004ELEC 121 Op Amps2 Basic Op-Amp The op-amp is a differential amplifier with a very high open loop gain.
Analog Electronics Lecture 5.
Analogue Electronics II EMT 212/4
Chapter 8 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
electronics fundamentals
09/16/2010© 2010 NTUST Today Course overview and information.
McGraw-Hill © 2008 The McGraw-Hill Companies Inc. All rights reserved. Electronics Principles & Applications Seventh Edition Chapter 7 More About Small-Signal.
Chapter 19 Electronics Fundamentals Circuits, Devices and Applications - Floyd © Copyright 2007 Prentice-Hall Chapter 19.
Chapter 14: Operational Amplifiers. Copyright ©2009 by Pearson Education, Inc. Upper Saddle River, New Jersey All rights reserved. Electronic Devices.
Electronics Fundamentals 8 th edition Floyd/Buchla © 2010 Pearson Education, Upper Saddle River, NJ All Rights Reserved. chapter 18 electronics.
9-1 McGraw-Hill © 2013 The McGraw-Hill Companies, Inc. All rights reserved. Electronics Principles & Applications Eighth Edition Chapter 9 Operational.
© 2012 Pearson Education. Upper Saddle River, NJ, All rights reserved. Electronic Devices, 9th edition Thomas L. Floyd Electronic Devices Ninth.
© 2013 The McGraw-Hill Companies, Inc. All rights reserved. McGraw-Hill 9-1 Electronics Principles & Applications Eighth Edition Chapter 9 Operational.
Microprocessor Interface
Lecture 1 Op-Amp Introduction of Operation Amplifier (Op- Amp) Analysis of ideal Op-Amp applications Comparison of ideal and non-ideal Op-Amp Non-ideal.
Microelectronic Circuits, Sixth Edition Sedra/Smith Copyright © 2010 by Oxford University Press, Inc. C H A P T E R 02 Operational Amplifiers.
Electronics Principles & Applications Fifth Edition Chapter 9 Operational Amplifiers ©1999 Glencoe/McGraw-Hill Charles A. Schuler.
10/11/2015 Operational Amplifier Characterization Chapter 3.
Operational Amplifiers AC Power CHAPTER 8. Figure 8.2, A voltage amplifier Figure 8.2 Simple voltage amplifier model Figure 8.3.
Module 4 Operational Amplifier
© 2013 The McGraw-Hill Companies, Inc. All rights reserved. McGraw-Hill 6-1 Electronics Principles & Applications Eighth Edition Chapter 6 Introduction.
Electronics Principles & Applications Fifth Edition Chapter 6 Introduction to Small-Signal Amplifiers ©1999 Glencoe/McGraw-Hill Charles A. Schuler.
© 2013 The McGraw-Hill Companies, Inc. All rights reserved. McGraw-Hill 6-1 Electronics Principles & Applications Eighth Edition Chapter 6 Introduction.
1 Fundamentals of Microelectronics  CH1 Why Microelectronics?  CH2 Basic Physics of Semiconductors  CH3 Diode Circuits  CH4 Physics of Bipolar Transistors.
OPERATIONAL AMPLIFIERS. BASIC OP-AMP Symbol and Terminals A standard operational amplifier (op-amp) has; V out is the output voltage, V+ is the non-inverting.
Basic Electronics Ninth Edition Basic Electronics Ninth Edition ©2002 The McGraw-Hill Companies Grob Schultz.
Chapter 30 Operational Amplifiers. 2 Introduction Characteristics –High input impedance –Low output impedance –High open-loop gain –Two inputs –One output.
0 Chap 2. Operational amplifiers (op-amps) Circuit symbol of an op-amp Widely used Often requires 2 power supplies + V Responds to difference between.
EE2301: Basic Electronic Circuit Amplifiers - Unit 1: Amplifier Model1 Block D: Amplifiers.
7-1 McGraw-Hill © 2013 The McGraw-Hill Companies, Inc. All rights reserved. Electronics Principles & Applications Eighth Edition Chapter 7 More About Small-Signal.
© 2013 The McGraw-Hill Companies, Inc. All rights reserved. McGraw-Hill 7-1 Electronics Principles & Applications Eighth Edition Chapter 7 More About Small-Signal.
© 2013 The McGraw-Hill Companies, Inc. All rights reserved. McGraw-Hill 8-1 Electronics Principles & Applications Eighth Edition Chapter 8 Large-Signal.
MALVINO Electronic PRINCIPLES SIXTH EDITION.
Electronics Principles & Applications Fifth Edition Chapter 8 Large-Signal Amplifiers ©1999 Glencoe/McGraw-Hill Charles A. Schuler.
Electronics Principles & Applications Fifth Edition Chapter 7 More About Small-Signal Amplifiers ©1999 Glencoe/McGraw-Hill Charles A. Schuler.
Differential Amplifiers
Exam 3 information Open book, open notes, bring a calculator Eligible topics (1 of 9) (not an exhaustive list) Generic amplifiers Amplifier basics voltage.
1 CHAPTER 20 OPERATIONAL AMPLIFIERS (OP-AMPS). 2 Introduction to operational amplifiers Symbol and Terminals.
1 Chapter 8 Operational Amplifier as A Black Box  8.1 General Considerations  8.2 Op-Amp-Based Circuits  8.3 Nonlinear Functions  8.4 Op-Amp Nonidealities.
PRESENTATION ON:  Voltage Amplifier Presentation made by: GOSAI VIVEK ( )
OPERATIONAL AMPLIFIERS + - Presented by D.Satishkumar Asst. Professor, Electrical & Electronics Engineering
1 Operational Amplifiers 1. 2 Outlines Ideal & Non-ideal OP Amplifier Inverting Configuration Non-inverting Configuration Difference Amplifiers Effect.
CHAPTER 20 OPERATIONAL AMPLIFIERS (OP-AMPS). Introduction to operational amplifiers Symbol and Terminals.
Module 2 Operational Amplifier Basics
Operational Amplifiers Chapter 10 Boylestad Electronic Devices and Circuit Theory.
Chapter 10: Operational Amplifiers
PUSAT PENGAJIAN KEJURUTERAAN KOMPUTER & PERHUBUNGAN
Analogue Electronics Circuit II EKT 214/4
Electronic Devices Ninth Edition Floyd Chapter 12.
Principles & Applications Operational Amplifiers
Presentation transcript:

Principles & Applications Operational Amplifiers Electronics Principles & Applications Sixth Edition Charles A. Schuler Chapter 9 Operational Amplifiers (student version) ©2003 Glencoe/McGraw-Hill

INTRODUCTION The Differential Amplifier The Operational Amplifier Determining Gain Frequency Effects Applications Comparators

Dear Student: This presentation is arranged in segments. Each segment is preceded by a Concept Preview slide and is followed by a Concept Review slide. When you reach a Concept Review slide, you can return to the beginning of that segment by clicking on the Repeat Segment button. This will allow you to view that segment again, if you want to.

Concept Preview Differential amplifiers always have two inputs. Differential amplifiers can have one or two outputs. Driving one input provides a difference signal. Both outputs will be active and will be out of phase with each other. Driving both inputs with the same signal results in reduced output. Driving both inputs with a difference signal results in increased output.

C C B B E E A differential amplifier driven at one input +VCC -VEE Inverted output Noninverted output +VCC C C B B E E -VEE

Both outputs are active because Q1 drives Q2. Q1 serves as an emitter-follower amplifier in this mode to drive Q2. Q2 serves as a common-base amplifier in this mode. It’s driven at its emitter. +VCC C C B B E E Q1 Q2 -VEE

C C B B E E A differential amplifier driven at both inputs +VCC -VEE Common mode input signal Reduced output Reduced output +VCC C C B B E E -VEE

C C B B E E A differential amplifier driven at both inputs +VCC -VEE Differential mode input signal Increased output Increased output +VCC C C B B E E -VEE

Concept Review Differential amplifiers always have two inputs. Differential amplifiers can have one or two outputs. Driving one input provides a difference signal. Both outputs will be active and will be out of phase with each other. Driving both inputs with the same signal results in reduced output. Driving both inputs with a difference signal results in increased output. Repeat Segment

Concept Preview The current in the emitter resistor divides equally between the two transistors in a differential amp. The differential gain is determined by the collector load and the ac emitter resistance. The common mode gain is determined by the collector load and the emitter resistor. The ratio of the differential gain to the common mode gain is called the CMRR. The CMRR is greatly improved by using a current source in the emitter circuit.

Differential Amplifier dc Analysis IRE = VEE - VBE RE 9 V - 0.7 V 3.9 kW = = 2.13 mA VRL = IC x RL = 1.06 mA x 4.7 kW IE = IRE 2 = 1.06 mA VCC +9 V = 4.98 V VCE = VCC - VRL - VE 4.7 kW RL RL 4.7 kW = 9 - 4.98 -(-0.7) IC = IE = 1.06 mA C C = 4.72 V B B E E 10 kW RB RB 10 kW 3.9 kW RE VEE -9 V

Differential Amplifier dc Analysis (continued) Assume b = 200 VB = VRB = IB x RB = 5.3 mA x 10 kW IB = IC b 1.06 mA 200 = VCC +9 V = 53 mV = 5.3 mA 4.7 kW RL RL 4.7 kW C C B B E E 10 kW RB RB 10 kW 3.9 kW RE VEE -9 V

Differential Amplifier ac Analysis 50 mV IE = 1.06 mA = 47 W (50 mV is conservative) VCC +9 V AV(CM) = RL 2 x RE AV(DIF) = RL 2 x rE 4.7 kW 2 x 3.9 kW = 4.7 kW RL RL 4.7 kW = 50 4.7 kW 2 x 47 W = C C = 0.6 B B E E 10 kW RB RB 10 kW 3.9 kW RE VEE -9 V

Differential Amplifier ac Analysis (continued) CMRR = 20 x log AV(DIF) AV(CM) = 20 x log 50 0.6 = 38.4 dB VCC +9 V 4.7 kW RL RL 4.7 kW C C B B E E 10 kW RB RB 10 kW 3.9 kW RE VEE -9 V

* C C B B E E A current source can replace RE to decrease the common mode gain. AV(CM) = RL 2 x RE VCC Replaces this with a very high resistance value. 4.7 kW RL RL 4.7 kW C C B B E E 10 kW RB RB 10 kW * 2 mA NOTE: Arrow shows conventional current flow.

A Practical Current Source IZ = 9 V - 5.1 V 390 W = 10 mA IC IE = = 2 mA 5.1 V - 0.7 V 2.2 kW 390 W IC = IE = 2 mA 5.1 V 2.2 kW -9 V

The common-mode signal cannot be seen in the output. A Demonstration of Common-mode Rejection The common-mode signal cannot be seen in the output. The amplitude of the common-mode signal is almost 30 times the amplitude of the differential signal. 6.3 V 60 Hz 212 mV 1 kHz

Differential Amplifier Quiz When a diff amp is driven at one input, the number of active outputs is _____. two When a diff amp is driven at both inputs, there is high gain for a _____ signal. differential When a diff amp is driven at both inputs, there is low gain for a ______ signal. common-mode The differential gain can be found by dividing the collector load by ________. 2rE The common-mode gain can be found by dividing the collector load by ________. 2RE

Concept Review The current in the emitter resistor divides equally between the two transistors in a differential amp. The differential gain is determined by the collector load and the ac emitter resistance. The common mode gain is determined by the collector load and the emitter resistor. The ratio of the differential gain to the common mode gain is called the CMRR. The CMRR is greatly improved by using a current source in the emitter circuit. Repeat Segment

Concept Preview Operational amplifiers have one output and two inputs: inverting and non-inverting. Some op amps have offset null terminals which can be used to zero the dc output. The output of an op can change no faster than its slew rate. Slew rate is specified in volts per microsecond. The slew rate and the amplitude of the output signal determine the power bandwidth of an op amp.

Op amps have two inputs Inverting input Output Non-inverting input

Op-amp Characteristics High CMRR High input impedance High gain Low output impedance Available as ICs Inexpensive Reliable Widely applied

With both inputs grounded through equal resistors, VOUT should be zero volts. +VCC VOUT Imperfections can make VOUT non-zero. The offset null terminals can be used to zero VOUT. -VEE

Dt DV DV Dt Slew rate = 741 0.5 V ms The output of an op amp cannot change instantaneously.

Slew-rate distortion VP f > fMAX fMAX = Slew Rate 2p x VP fMAX is known as the power bandwidth.

Operational Amplifier Quiz The input stage of an op amp is a __________ amplifier. differential Op amps have two inputs: one is inverting and the other is ________. noninverting An op amp’s CMRR is a measure of its ability to reject a ________ signal. common-mode The offset null terminals can be used to zero an op amp’s __________. output The ability of an op amp output to change rapidly is given by its _________. slew rate

Concept Review Operational amplifiers have one output and two inputs: inverting and non-inverting. Some op amps have offset null terminals which can be used to zero the dc output. The output of an op can change no faster than its slew rate. Slew rate is specified in volts per microsecond. The slew rate and the amplitude of the output signal determine the power bandwidth of an op amp. Repeat Segment

Concept Preview An op amp follower has a closed loop gain of 1. The input and output signals are in-phase in a follower amplifier. The closed loop gain can be increased by decreasing the feedback ratio. The input and output signals are out of phase in an inverting amplifier. The – terminal of an inverting amplifier acts as a virtual ground. The input impedance of an inverting amplifier is equal to the input resistor.

It has a high input impedance and a low output impedance. Op-amp Follower AV(OL) = the open loop voltage gain AV(CL) = the closed loop voltage gain This is a closed-loop circuit with a voltage gain of 1. It has a high input impedance and a low output impedance. RL

The differential input Op-amp Follower AV(OL) = 200,000 AV(CL) = 1 The differential input approaches zero due to the high open-loop gain. Using this model, VOUT = VIN. VDIF = 0 VOUT RL VIN

Op-amp Follower AV(OL) = 200,000 B = 1 AB +1 A VIN VOUT The feedback ratio = 1 200,000 (200,000)(1) + 1 @ 1 AV(CL) = VOUT RL VIN

The closed-loop gain is increased by decreasing the feedback with a voltage divider. 200,000 (200,000)(0.091) + 1 = 11 AV(CL) = RF B = R1 RF + R1 100 kW R1 10 kW 10 kW 100 kW + 10 kW = VOUT RL VIN = 0.091

It’s possible to develop a different model for the closed loop gain by assuming VDIF = 0. VIN = VOUT x R1 R1 + RF RF Divide both sides by VOUT and invert: 100 kW R1 10 kW = VOUT VIN 1 + RF R1 VDIF = 0 VOUT RL VIN AV(CL) = 11

-VOUT -RF In this amplifier, the assumption VDIF = 0 leads to the conclusion that the inverting op amp terminal is also at ground potential. This is called a virtual ground. We can ignore the op amp’s input current since it is so small. Thus: Virtual ground RF IR1 = IRF 10 kW 1 kW By Ohm’s Law: R1 VIN R1 = -VOUT RF VDIF = 0 VIN VOUT RL VOUT VIN = -RF R1 = -10 The minus sign designates an inverting amplifier.

Due to the virtual ground, the input impedance of the inverting amplifier is equal to R1. Virtual ground RF Although op amp input currents are small, in some applications, offset error is minimized by providing equal paths for the input currents. 10 kW R1 1 kW VDIF = 0 VIN R2 = R1 || RF = 910 W This resistor reduces offset error.

Concept Review An op amp follower has a closed loop gain of 1. The input and output signals are in-phase in a follower amplifier. The closed loop gain can be increased by decreasing the feedback ratio. The input and output signals are out-of-phase in an inverting amplifier. The – terminal of an inverting amplifier acts as a virtual ground. The input impedance of an inverting amplifier is equal to the input resistor. Repeat Segment

Concept Preview Most op amps have built-in frequency compensation. The internal frequency compensation produces a break frequency of 10 Hz or so. The closed loop small signal bandwidth is greater than the break frequency. A Bode plot can be used to determine the small signal bandwidth of a closed loop amplifier. The gain-bandwidth product can also be used to determine the closed loop small signal bandwidth.

A typical op amp has internal frequency compensation. Output C Break frequency: fB = 2pRC 1

Bode Plot of a Typical Op Amp Break frequency 120 100 80 60 Gain in dB 40 20 1 10 100 1k 10 k 100 k 1M Frequency in Hz

Op amps are usually operated with negative feedback (closed loop). This increases their useful frequency range. = VOUT VIN 1 + RF R1 AV(CL) = RF = 1 + 100 kW 1 kW = 101 100 kW R1 1 kW dB Gain = 20 x log 101 = 40 dB VOUT RL VIN

Using the Bode plot to find closed-loop bandwidth: 120 100 Gain in dB 80 Break frequency 60 AV(CL) 40 20 1 10 100 1k 10 k 100 k 1M Frequency in Hz

There are two frequency limitations: 0.5 V ms 70 V ms A 741 op amp slews at A 318 op amp slews at There are two frequency limitations: Slew rate determines the large-signal bandwidth. Internal compensation sets the small-signal bandwidth.

The Bode plot for a fast op amp shows increased bandwidth. 120 100 fUNITY is also called the gain-bandwidth product. 80 Gain in dB 60 40 fUNITY 20 1 10 100 1k 10 k 100 k 1M 10M Frequency in Hz

fUNITY can be used to find the small-signal bandwidth. = VOUT VIN 1 + RF R1 AV(CL) = RF = 1 + 100 kW 1 kW = 101 100 kW R1 1 kW fB = fUNITY AV(CL) VOUT RL VIN 318 Op amp 10 MHz 101 = 99 kHz =

Op Amp Feedback Quiz The open loop gain of an op amp is reduced with __________ feedback. negative The ratio RF/R1 determines the gain of the ___________ amplifier. inverting 1 + RF/R1 determines the gain of the ___________ amplifier. noninverting Negative feedback makes the - input of the inverting circuit a ________ ground. virtual Negative feedback _________ small signal bandwidth. increases

Concept Review Most op amps have built-in frequency compensation. The internal frequency compensation produces a break frequency of 10 Hz or so. The closed loop small signal bandwidth is greater than the break frequency. A Bode plot can be used to determine the small signal bandwidth of a closed loop amplifier. The gain-bandwidth product can also be used to determine the closed loop small signal bandwidth. Repeat Segment

Concept Preview The amplitude response of an RC lag network is –20 dB per decade beyond the break frequency. The phase response of an RC lag network is –45 degrees at the break frequency. The Miller effect makes some interelectrode capacitances appear to be larger. Multiple lag networks inside an op amp make negative feedback become positive at some frequency. Frequency compensation insures that the gain is less than 0 dB at that frequency.

Amplitude Response of RC Lag Circuit Vout C fb = 2pRC 1 fb 10fb 100fb 1000fb f 0 dB -20 dB Vout -40 dB -60 dB

Phase Response of RC Lag Circuit Vout C R -XC  = tan-1 0.1fb fb 10fb 0o f Vout -45o -90o

Interelectrode Capacitance and Miller Effect The gain from base to collector makes CBC effectively larger in the input circuit. CBC CBE R CMiller CBE CMiller = AVCBC fb = 2pRCInput 1 CInput = CMiller + CBE

Bode Plot of an Amplifier with Two Break Frequencies 50 dB 40 dB 20 dB/decade 30 dB 20 dB 40 dB/decade 10 dB 0 dB 10 Hz 100 Hz 1 kHz 10 kHz 100 kHz fb1 fb2

Multiple Lag Circuits: Vout R1 R2 R3 C1 C2 C3 0o f Vout Phase reversal -180o Negative feedback becomes positive!

Op Amp Compensation Interelectrode capacitances create several break points. Negative feedback becomes positive at some frequency due to cumulative phase lags. If the gain is > 0 dB at that frequency, the amplifier is unstable. Frequency compensation reduces the gain to 0 dB or less.

Op Amp Compensation Quiz Beyond fb, an RC lag circuit’s output drops at a rate of __________ per decade. 20 dB The maximum phase lag for one RC network is __________. 90o An interelectrode capacitance can be effectively much larger due to _______ effect. Miller Op amp multiple lags cause negative feedback to be ______ at some frequency. positive If an op amp has gain at the frequency where feedback is positive, it will be ______. unstable

Concept Review The amplitude response of an RC lag network is –20 dB per decade beyond the break frequency. The phase response of an RC lag network is –45 degrees at the break frequency. The Miller effect makes some interelectrode capacitances appear to be larger. Multiple lag networks inside an op amp make negative feedback become positive at some frequency. Frequency compensation insures that the gain is less than 0 dB at that frequency. Repeat Segment

Concept Preview Op amps can be used to sum (add) two or more signals. Scaling in a summing amp provides different gain for each signal. Op amps can be used to subtract two signals. Cascade RC filters have relatively poor performance. Active filters combine op amps with RC networks. Feedback in an op amp active filter sharpens the knee of the frequency response curve.

RF Summing Amplifier Amplifier scaling: 1 kHz signal gain is -10 Inverted sum of three sinusoidal signals RF 5 kHz 5 kW 10 kW Summing Amplifier 3.3 kW Amplifier scaling: 1 kHz signal gain is -10 3 kHz signal gain is -3 5 kHz signal gain is -2 3 kHz 1 kW 1 kHz

common-mode rejection) Difference of two sinusoidal signals (V1 = V2) RF 1 kW Subtracting Amplifier (A demonstration of common-mode rejection) 1 kW VOUT = V2 - V1 1 kW 1 kW V1 V2

A cascade RC low-pass filter (A poor performer since later sections load the earlier ones.) An active low-pass filter (The op amps provide isolation and better performance.)

Active filter -20 Cascade RC -40 Amplitude in dB -60 10 100 Frequency in Hz

Active low-pass filter with feedback VOUT C1 C2 VIN feedback At relatively low frequencies, Vout and Vin are about the same. Thus, the signal voltage across C1 is nearly zero. C1 has little effect at these frequencies.

Active low-pass filter with feedback VOUT C1 C2 VIN As fIN increases and C2 loads the input, Vout drops. This increases the signal voltage across C1. This sharpens the knee. -3 dB Feedback can make a filter’s performance even better! Gain Frequency fC

The slope eventually reaches 24 dB/octave or 80 db/decade Note the flat pass band and the sharp knee. Active filter using feedback (two stages) -20 -40 Amplitude in dB The slope eventually reaches 24 dB/octave or 80 db/decade for all the filters (4 RC sections). -60 10 100 Frequency in Hz

Concept Review Op amps can be used to sum (add) two or more signals. Scaling in a summing amp provides different gain for each signal. Op amps can be used to subtract two signals. Cascade RC filters have relatively poor performance. Active filters combine op amps with RC networks. Feedback in an op amp active filter sharpens the knee of the frequency response curve. Repeat Segment

Concept Preview Other active filters include high-pass, band-pass and band-stop. An active rectifier will work with millivolt level signals. The output slope of an op amp integrator is equal to the dc input voltage times the reciprocal of the time constant. Comparators can be used to change analog waveforms to digital waveforms. A Schmitt trigger uses positive feedback to produce hysteresis and noise immunity.

Active high-pass filter VOUT VIN feedback -3 dB Gain fC Frequency

Active band-pass filter VIN VOUT Active band-pass filter (multiple feedback) -3 dB Gain Frequency Bandwidth

Active band-stop filter VOUT VIN Active band-stop filter (multiple feedback) -3 dB Gain Frequency Stopband

0 V 56.6 mV Active rectifier 40 mV 0 V - 56.6 mV

Integrator C V Slope = s R VOUT VIN Slope = -VIN x 1 RC

Comparator with a 1 Volt Reference +VSAT 1 V 0 V -VSAT VOUT VIN 1 V

Comparator with a Noisy Input Signal +VSAT 1 V 0 V -VSAT VOUT VIN 1 V

Schmitt Trigger with a Noisy Input Signal +VSAT UTP LTP -VSAT Trip points: R1 + RF R1 VSAT x VOUT VIN RF R1 Hysteresis = UTP - LTP

VOUT is LOW (0 V) when VIN is between 1 V and 3 V. Window Comparator 4.7 kW R1 311 VOUT VUL 3 V R2 4.7 kW VIN 311 VLL VOUT is LOW (0 V) when VIN is between 1 V and 3 V. 1 V

require pull-up resistors in applications of this type. +5 V Window Comparator 311 VOUT VUL 3 V VIN 311 Many comparator ICs require pull-up resistors in applications of this type. VLL 1 V

VOUT is TTL logic compatible. Window Comparator 4.7 kW R1 311 VOUT VUL 3 V R2 4.7 kW VIN 311 VLL VOUT is TTL logic compatible. 1 V

Op Amp Applications Quiz A summing amp with different gains for the inputs uses _________. scaling Frequency selective circuits using op amps are called _________ filters. active An op amp integrator uses a _________ as the feedback element. capacitor A Schmitt trigger is a comparator with __________ feedback. positive A window comparator output is active when the input is ______ the reference points. between

Concept Review Other active filters include high-pass, band-pass and band-stop. An active rectifier will work with millivolt level signals. The output slope of an op amp integrator is equal to the dc input voltage times the reciprocal of the time constant. Comparators can be used to change analog waveforms to digital waveforms. A Schmitt trigger uses positive feedback to produce hysteresis and noise immunity. Repeat Segment

REVIEW The Differential Amplifier The Operational Amplifier Determining Gain Frequency Effects Applications Comparators